Author Affiliations
Abstract
Solid State Laser Laboratory, Center for Physical Sciences and Technology, Vilnius, Lithuania
We present a compact and cost-effective mJ-level femtosecond laser system operating at a center wavelength of approximately 2.15 μm. An affordable two-stage ytterbium-doped yttrium aluminum garnet (Yb:YAG) chirped pulse amplifier provides more than 10 mJ, approximately 1.2 ps pulses at 1030 nm to pump a three-stage optical parametric chirped pulse amplifier (OPCPA) based on bismuth borate crystals and to drive the supercontinuum seed in the YAG crystal. The energy of the amplified pulses in the wavelength range of 1.95–2.4 μm reached 2.25 mJ with a pump-to-signal conversion efficiency of approximately 25% in the last OPCPA stage. These pulses were compressed to 38 fs in a pair of Suprasil 300 glass prisms.
mid-infrared optical parametric chirped pulse amplifier short infrared supercontinuum ytterbium-doped yttrium aluminum garnet 
High Power Laser Science and Engineering
2023, 11(2): 02000e27
Author Affiliations
Abstract
School of Physics and Astronomy, Key Laboratory for Laser Plasmas (Ministry of Education), Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University, Shanghai, China
We report on a grating-free fiber chirped pulse amplifier (CPA) at 2.8 μm for the first time. The CPA system adopted Er:ZBLAN fiber with large anomalous dispersion as the stretcher and germanium (Ge) rods as the compressor with a compact structure. High-energy picosecond pulses of 2.07 μJ were generated at the repetition rate of 100 kHz. Using highly dispersive Ge rods, the amplified pulses were compressed to 408 fs with a pulse energy of 0.57 μJ, resulting in a peak power of approximately 1.4 MW. A spectral broadening phenomenon in the main amplifier was observed, which was caused by the special gain shape of the Er:ZBLAN fiber amplifier in operation and confirmed by our numerical simulation. This compact fiber CPA system at 2.8 μm will be practical and meaningful for application fields.
Er:ZBLAN fiber fiber chirped pulse amplifier grating free mid-infrared 
High Power Laser Science and Engineering
2022, 10(6): 06000e41
冯天利 1,2,3,*商景诚 1,2,3李涛 1,2,3
作者单位
摘要
1 山东大学信息科学与工程学院,山东 青岛 266237
2 山东大学山东省激光技术与应用重点实验室,山东 青岛 266237
3 山东大学激光与红外系统集成技术教育部重点实验室,山东 青岛 266237
报道了一种包含两个激光成丝过程的工作在2 μm波段的光参量啁啾脉冲放大(OPCPA)系统前端,该前端工作在简并模式下,2 μm种子激光脉冲通过近红外和可见光波段的超连续光谱之间差频产生。可见光和近红外波段的超连续光谱分别通过泵浦脉冲激光在两个YAG晶体中通过激光成丝过程产生。经过光参量放大及合理的色散补偿后,2 μm种子激光脉冲的波长可从1830 nm覆盖至2320 nm,脉冲宽度为29 fs,单脉冲能量为16.7 μJ,平均功率为167 mW,功率波动小于3%。
非线性光学 光参量啁啾脉冲放大器 激光成丝 2 μm激光 差频产生 
中国激光
2022, 49(7): 0708002
商景诚 1,2,3刘一州 1,2赵圣之 1,2冯天利 1,2,3,*[ ... ]李涛 1,2,3,**
作者单位
摘要
1 山东大学信息科学与工程学院, 山东 青岛 266237
2 山东大学山东省激光技术与应用重点实验室, 山东 青岛 266237
3 山东大学激光与红外系统集成技术教育部重点实验室, 山东 青岛 266237
4 山东大学晶体材料研究所, 山东 济南 250100
光参量啁啾脉冲放大器(OPCPA)在实现高功率、大能量、光学周期量级的超短激光脉冲输出方面极具优势。对具有高脉冲重复频率(≥1 kHz)的OPCPA系统展开研究讨论,全面介绍OPCPA系统的组成;针对不同波段的OPCPA系统,对泵浦源、前端、光参量放大级和压缩器等关键模块分别进行对比和讨论,对限制OPCPA系统性能提升的因素进行分析;最后总结不同输出波长的高重复频率OPCPA系统的研究现状,并对未来的发展方向进行展望。
激光技术 光参量啁啾脉冲放大器 超快激光 高功率 高重复频率 光学周期 
中国激光
2021, 48(12): 1201004
Author Affiliations
Abstract
1 National Laboratory on High Power Laser and Physics , Shanghai Institute of Optics and Fine Mechanics , Chinese Academy of Sciences , Shanghai 201800 , China
2 University of Chinese Academy of Sciences , Beijing 100049 , China
We present the design and experiment of a broadband optical parametric chirped-pulse amplifier (OPCPA) which provides high conversion efficiency and good beam quality at 808 nm wavelength. Using a three-dimensional spatial and temporal numerical model, several design considerations necessary to achieve high conversion efficiency, good beam quality and good output stability are discussed. To improve the conversion efficiency and broaden the amplified signal bandwidth simultaneously, the nonlinear crystal length and OPCPA parameters are analyzed and optimized with the concept of dissipating amplified idler between optical parametric amplification (OPA) of two crystals configuration. In the experiment, an amplifier consisting of two OPCPA stages of ‘L’ type configuration was demonstrated by using the optimized parameters. An amplified signal energy of 160 mJ was achieved with a total pump-to-signal efficiency of 35% (43% efficiency for the OPCPA stage 2). The output bandwidth of signal pulse reached 80 nm and the signal pulse was compressed to 24 fs. The energy stability reached 1.67% RMS at 3% pump energy variation. The optimized OPCPA amplifier operates at a repetition rate of 1 Hz and is used as a front-end injection for the main amplifier of SG-II 5PW laser facility.
BBO nonlinear optics optical parametric chirped-pulse amplifier petawatt laser 
High Power Laser Science and Engineering
2018, 6(4): 04000e58
作者单位
摘要
1 北京大学人工微结构和介观物理国家重点实验室, 北京 100871
2 北京大学区域光纤通信网与新型光通信系统国家重点实验室, 北京 100871
研究了不同厚度周期极化铌酸锂晶体(PPLN)对掺铒飞秒光纤激光器倍频特性的影响。基于非线性偏振旋转锁模原理和啁啾脉冲放大技术,在1560 nm波段实现了重复频率为100 MHz,输出功率为423 mW,脉冲宽度为80 fs的掺铒飞秒光纤激光输出。以此为基频光源,对0.5,1,10 mm三种不同厚度PPLN倍频晶体进行倍频特性研究,实现了波长在780 nm的飞秒激光输出。其中采用0.5 mm晶体时获得了功率为100.4 mW、脉冲宽度为104 fs的倍频光输出,倍频转换效率为23.7%;采用1 mm晶体时获得了功率为165.0 mW、脉冲宽度为161 fs的倍频输出,倍频转换效率为39%;采用10 mm晶体时获得了功率为185.5 mW,脉冲宽度为305 fs的倍频光输出,倍频转换效率达43.7%。并解释了倍频转换效率和倍频光脉冲宽度随PPLN晶体厚度的变化规律。实验数据为基于锁模光纤激光器产生780 nm波段飞秒光脉冲的研究提供了有益的参考。
激光器 掺铒飞秒光纤激光器 啁啾脉冲放大器 非线性偏振旋转锁模 倍频 周期极化铌酸锂晶体 
中国激光
2018, 45(7): 0701001
作者单位
摘要
中国科学院上海光学精密机械研究所强光光学开放实验室,上海 201800
介绍了新近提出的光学啁啾脉冲参量放大技术,并以高增益、宽谱带的双轴非线性晶体LBO为例,研究了抽运光和信号光的相位匹配角的关系、增益、增益带宽、匹配角的选择,以及增益随晶体长度变化的趋势和双曲正割和高斯脉冲输入非线性晶体前后变化的情况。
双轴晶体 非线性 啁啾脉冲参量放大 
光学学报
2000, 20(9): 1153

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